OCP 5253--Introduction to Geophysical Fluid Dynamics
Recommend Documents
Fall 2012. Tuesdays, 9:00 am - 10:50 am, Warren Weaver Hall 517. Instructor.
Edwin Gerber gerber[at]cims.nyu.edu (e-mail is the best way to reach me).
Apr 5, 2011 ... Geophysical fluid dynamics is the study of the dynamics of fluid systems ... In the
geophysical context, the major body force is the conservative ...
Nov 18, 2012 ... Hamiltonian geophysical fluid dynamics. Ted Shepherd. Department of
Meteorology. University of Reading. FDEPS 2012, Lecture 2 ...
Feb 7, 2013 ... Geophysical Fluid Dynamics. Physical and Numerical Aspects. Benoit Cushman-
Roisin and Jean-Marie Beckers. Numerical Exercises Solution ...
Oct 31, 2014 - bootstrap resampling upon the original .... seasonal SST grids were converted to anomalies, ..... noaa.gov/psd/data/gridded/data.gpcp.html).
Nov 1, 1985 - A more direct proof of orthogonality is also available. The eigenvalue equation .... If we add a small scale-selective damp- ing of vorticity to the ...
6S 6 68. 62[(KH+ as) 62] (3) where t is time and z the vertical coordinate; z = 0 will ..... of the proï¬le on a vertical plane normal to the ice leading edge. The.
May 5, 1975 - Q. 90 60/ ,-. \l/ 1897 @D i so\ 336 10 Boï¬/ï¬o \~IO LE. 7 2o \ I .500â ..... holding capacity of the model atmosphere with time. In order to economize ...
Nov 15, 1989 - worth and McIntyre 1.985, for a review of critical layer theory). One is led to the hypothesis that the existence of a simple asymmetric life cycle of ...
the descending branch of Hadley cell and dry air ad- vecting out from the colder continent. Although ECHAM4 qualitatively simulates most of the above features, ...
5 a 0.4 0.4. 0.1 0.2 0.21 of f .i o i. 0 5 10 15 20 25 50 5 1o 15 20 25 50. 1.2 1.2 m 1< b 1. 0 Z5-55ï¬,5â15N ZWW.7â15N. 3 00+ 00+. 3 0.0 0.0. 5 g, 0.4 o.4~ h].
... water masses from which it originated. This level of saliniï¬cation is nowhere near the 0.9 unit in ...... SON SON 30N E0 303 505. 2000;. 3000â 5. ' DEPTH (m).
MONTHLY WEATHER REVIEW ... and Oceanic Sciences, Princeton University, Princeton, New Jersey .... climatological monthly mean SST data were used. By.
Treatment of Earth as an Inertial Frame in Geophysical Fluid Dynamics. Dana
Duke. PHGN 505 Term Paper. December 2011 ...
6S 6 68. 62[(KH+ as) 62] (3) where t is time and z the vertical coordinate; z = 0 will ..... of the proï¬le on a vertical plane normal to the ice leading edge. The.
Jan 4, 1996 - Geophysical Fluid Dynamics Laboratoty/NOAA, Princeton, New Jersey. (Manuscript .... The GFDL dataset of monthly mean variables and.
AVHRR channel spectral responses and descriptions (after Kidwell 1991). Central wavenumber. (cm'). Central wavelength. (microns). Approximate peak in.
Sigma Coordinate Pressure Gradient Errors and the Seamount Problem ... gradients on a sigma coordinate grid, prognostically disappeared, leaving behind a ...
Aug 19, 2006 - Trans-polar vgp shifts and earth's rotation. Nils-Axel Mörner a a. Paleogeophysics ... Because these shifts are recorded from different places on.
modulation of the Walker circulation by the ENSO events are key players in ...... Nevertheless, it is still useful to analyze this regime, since it reveals some new ..... the matrix AT A. In more general cases the answer is derived by solving ......
Oct 1, 1992 - guidance as to the dependence on temperature gra- vertical shear, (U(H) â U(0))/H. .... In the absence of the damping terms, baroclinic insta-.
Aug 7, 2009 - terms of derivatives of information entropy with respect to large ... Additionally we find that small scale turbulence systematically drives up .... the science of GFD provides the dynamic core for GCMs by writing (3) ..... The answer i
Finite depth stratified flow over topography on a beta-plane. E. R. Johnsona a Department of Mathematics, University of British Columbia, Vancouver, Canada.
OCP 5253--Introduction to Geophysical Fluid Dynamics
OCP 5253--Introduction to Geophysical Fluid Dynamics. Course Syllabus, Fall
Semester, 2013 (revised 8/23 2013). Tentatively scheduled for Wed 11:15- 2:00 ...
OCP 5253--Introduction to Geophysical Fluid Dynamics Course Syllabus, Fall Semester, 2013 (revised 8/23 2013) Tentatively scheduled for Wed 11:15- 2:00 pm. Exact time will be arranged during the first meeting; Room 327 OSB Instructor: Professor Doron Nof, 419 OSB OFFICE HOURS Tu/Thu 14:00 – 15:00
Dept Ph 644-6700; Direct Ph 644-2736
Course Description: The purpose of this first-year graduate class is to introduce the student to the basic principles governing the motion of fluids on a planetary scale. The primary effects that will be discussed are the effects of rotation and stratification on fluid motions. The focus will be on motions in oceans and atmospheres (on earth and other planets). The class is usually supplemented with actual demonstrations of fluid motions, many of which fit directly over a modified overhead projector. Some examples are, Coriolis deflections, Taylor curtains, Taylor columns, Taylor-Proudman theorem, bottom Ekman Layers, Sverdrup balance, and windinduced separation and its relationship to the Parson’s model. Textbooks: The class will be based on Introduction to Geophysical Fluid Dynamics” (Second Edition) by Professor Benoit Cushman-Roisin and Jean-Marie Beckers (Academic Press 2011), with occasional supplements from Stern’s Ocean Circulation Physics, Salmon’s Lectures on Geophysical Fluid Dynamics and Pedlosky’s Geophysical Fluid Dynamics. Lecture and Course Outline: 1. Introduction a. b. c. d. e. f.
Objective Importance of geophysical fluid dynamics Scales of motion Importance of rotation Importance of stratification Important distinctions between the oceans and atmosphere
2. The Coriolis Force a. b. c. d. e.
Motivation for the choice of a rotating reference framework Rotating frame of reference Unimportance of the centrifugal force Motion of a free particle on a rotating plane Acceleration on a three-dimensional rotating earth
3. The Governing Equations
a. b. c. d. e. f.
Momentum equations Other governing equations The Boussinesq approximation Further simplifications The equations governing geophysical flows The Rossby and Ekman numbers
4. Geostrophic Flows and Vorticity Dynamics a. b. c. d.
Homogeneous geostrophic flows Homogeneous geostrophic flows over an irregular bottom (Taylor columns) Generalization to non-geostrophic flows Vorticity dynamics
5. The Ekman Layer a. b. c. d. 6.
The importance of friction The bottom Ekman layer The surface Ekman layer The Ekman layer in real geophysical flows
Geostrophic adjustment a. The simplest adjustment problem (a wall pushed sideways) b. The full adjustment problem c. The collapsing cylinder d. The collapsing wedge
7.
Large-Scale Ocean Circulation a. A simple model of mid-latitude circulation b. Sverdrup transport c. Westward intensification
8.
Layered models a. Two layers “reduced gravity” models b. Parson’s separation model c. Analogy between the Parson’s model and wind set-up in a lake d. Analogy between Parson’s model and the thermocline structure along the equatorial Pacific
There will be several homework assignments and a set of exams whose specifics will be determined in the first meeting with students input. The final grade will be determined on the basis of homework evaluation (10%) and the exam(s) grade (90%). Occasionally, the lectures
will be supplemented with various videos of relevant laboratory experiments. Students are reminded that the university has an Academic Honor Code (described in the Student Handbook).